EP0566640B1 - Justierungsvorrichtung für resonanzmodul - Google Patents

Justierungsvorrichtung für resonanzmodul Download PDF

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Publication number
EP0566640B1
EP0566640B1 EP92903213A EP92903213A EP0566640B1 EP 0566640 B1 EP0566640 B1 EP 0566640B1 EP 92903213 A EP92903213 A EP 92903213A EP 92903213 A EP92903213 A EP 92903213A EP 0566640 B1 EP0566640 B1 EP 0566640B1
Authority
EP
European Patent Office
Prior art keywords
signal
frequency
voltage
oscillator
resonance
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Expired - Lifetime
Application number
EP92903213A
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English (en)
French (fr)
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EP0566640A1 (de
Inventor
Lennart Larsson
Ulf Saldell
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Allgon AB
Original Assignee
Allgon AB
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Publication date
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Publication of EP0566640A1 publication Critical patent/EP0566640A1/de
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Classifications

    • H—ELECTRICITY
    • H03—ELECTRONIC CIRCUITRY
    • H03J—TUNING RESONANT CIRCUITS; SELECTING RESONANT CIRCUITS
    • H03J7/00—Automatic frequency control; Automatic scanning over a band of frequencies
    • H03J7/02—Automatic frequency control
    • H03J7/16—Automatic frequency control where the frequency control is accomplished by mechanical means, e.g. by a motor
    • H—ELECTRICITY
    • H03—ELECTRONIC CIRCUITRY
    • H03L—AUTOMATIC CONTROL, STARTING, SYNCHRONISATION OR STABILISATION OF GENERATORS OF ELECTRONIC OSCILLATIONS OR PULSES
    • H03L7/00—Automatic control of frequency or phase; Synchronisation
    • H03L7/06—Automatic control of frequency or phase; Synchronisation using a reference signal applied to a frequency- or phase-locked loop

Definitions

  • the present invention relates to an arrangement in tuning resonance modules including a cavity and resonance body, which is steered to a resonance position by a motor driven by a voltage as long as there is a phase difference between the input signal to the resonance module and its output signal, called the measuring signal, the input signal being of high frequency
  • Fig. 1 is a circuit diagram in accordance with the invention.
  • Fig. 2 schemayically illustrates the frequency as a function of phase angle.
  • Fig. 3 schematically illustrates the transposition of signal high frequency to low frequency for the same signal.
  • the letter A denotes a collection point on an antenna, where four signals of different frequencies are collected for common transmission from the antenna B.
  • a signal 4' is sent from the resonance module 2.
  • a transmitter is denoted by the letters PA, and a signal from it goes to an isolator 1 and further to the resonance module 2.
  • the latter is formed with a cavity accommodating a movable resonance means driven by a motor until resonance occurs between the reference signal and the signal (called the measuring signal) coming from the module. Since the latter does not form any part of the invention it is not described further.
  • the isolator 1 solely permits passage of signals in the mentioned direction, and prevents any signal reflected in the module, as well as signals from the collection point A and through the module from reaching the transmitter PA.
  • a reference signal is taken from the input at a point C.
  • an attenuator 3 for adjusting the signal to a level suitable to a mixer 4.
  • the signal thus arrives at the mixer, and this reference signal from the attentuator is then mixed with an output signal from an oscillator 5.
  • the mixer 4 gives one signal, which is the sum of the two input signals, and one which is the difference between the two signals.
  • a bandpass filter 6 which is formed for passing through the signal constituting the difference between the two input signals to the mixer 4.
  • the output signal from the mixer will be of low frequency and can pass through the bandpass filter 6. This can provide the lowest possible frequency, e.g. 20 to 220 kHz. These values should be viewed in relation to the frequency of the input signal from PA, which can be about 1000 MHz.
  • the bandpass filter there is an attenuator 7, and this, together with an amplifier 8, determines a power range suitable for the system. There is thus obtained after the attentuator 7 and limiting amplifier 8 an output signal with a constant amplitude, irrespective of the input amplitude, within a power range normal for the system.
  • a phase detector 16 and a lopass filter 15 together form a wideband frequency detector.
  • An integrator circuit 17 compares the output voltage of the frequency detector 15,16 with a reference voltage at a point 18 in this circuit. The output signal of the integrator circuit is taken via a line 20 to the oscillator 5, so that the difference frequency in this case is given a mean value of 120 kHz (see Fig. 2), the reference voltage having been selected at 2.5 V.
  • the oscillator 5 is voltage controlled, so that a higher voltage gives a higher frequency and a lower voltage a lower frequency.
  • the oscillator may have a sensitivity of 14 MHz per volt. Accordingly, when the frequency detector 16 has shifted the reference voltage 90 degrees, so that the output voltage will be equal to the reference voltage, this will mean that the voltage in the signal through the line 20 is constant, thus giving an output signal from the oscillator that is constant at a value somewhere between 90 MHz and 1000 MHz.
  • the attenuator determines the difference between the signal coming from the oscillator and the reference signal, it will be understood that the output signal from the attenuator has a low frequency, which will be lower the nearer the oscillator frequency is to the reference signal frequency.
  • a signal is also taken to a second phase detector 9, which compares the phase difference of the reference signal processed in the means 3-8 with a measuring signal coming from a directional coupler 10.
  • an attenuator 11 of the same kind as attenuator 3, is disposed in the line from the directional coupler.
  • the signal from the attenuator goes to a second mixer 12, similar to the mixer 4, for further propagation of the difference between the signal from oscillator 5 and the signal from the attenuator 11.
  • a bandpass filter 13 sorts out three of the signals from the mixer 12, and in this case the signal 4' is taken to the phase detector 9 via a limiting amplifier 14.
  • Fig. 3 illustrates the transposition of the transmitter frequency, including its modulation, e.g. to a value within the 900 MHz - 1000 MHz range, to a mean value of about 120 kHz.
  • the oscillator sweeps from right to left (see the arrow vco), and that the signals 1', 2', 3' are filtered off in the bandpass filter 13, since their frequencies are far away from the frequency of 4', see the upper part of Fig. 3.
  • a "new" signal is obtained by forming the difference between the frequencies of the reference and oscillator signals, and this signal has a frequency that will be lower the less the difference is between the frequencies of the two signals just mentioned. This is illustrated by the middle frequency scale in Fig. 3, where the newly formed signal is situated, e.g. with a frequency range of 200 kHz (Fig. 3, bottom part).
  • phase detector 9 gives an output voltage if there is a phase difference, and this voltage is compared with a reference voltage 22 in an integrator 21, the output voltage of which drives an adjusting motor M. It is this motor M that drives the unillustrated resonance body of the resonance module 2 to the position where resonance is obtained, i.e. when the difference between input and output signal to an from the module is zero.
  • the oscillator has been described hereinbefore as an important item in the invention, since it shall, with the aid of the mixer, give the low-frequency signal. It has also been described above how the oscillator is controlled by a voltage determined by the reference signal and a reference voltage. The oscillator voltage may be decided in another way, however.
  • the reference signal could be taken directly from the transmitter, and via a modulating means it could be given a somewhat deviating frequency, which is allowed to decide the oscillator's corresponding frequency.
  • Another method is to control the oscillator with the aid of a digital code from the transmitter, via a frequency synthesizing circuit.

Landscapes

  • Transmitters (AREA)
  • Stabilization Of Oscillater, Synchronisation, Frequency Synthesizers (AREA)
  • Radar Systems Or Details Thereof (AREA)
  • Steering Control In Accordance With Driving Conditions (AREA)
  • Measurement Of Resistance Or Impedance (AREA)

Claims (6)

  1. Anordnung in Abstimmungs-Resonanzmodulen, die einen Hohlraum und einen Resonanzkörper aufweisen, der zu einer Resonanzposition gesteuert wird durch einen Motor, der durch eine erste Spannung angetrieben ist, solange es eine Phasendifferenz zwischen einem Hochfrequenz-Eingangssignal zu dem Resonanzmodul und einem Ausgangssignal davon, Meßsignal genannt, gibt, dadurch gekennzeichnet, daß die Anordnung einen Hochfrequenzoszillator (5) aufweist, der durch eine zweite Spannung gesteuert ist und einen Frequenzbereich hat, in dem die Frequenz des Eingangssignals liegt; daß die Differenz zwischen dem Ausgangssignal von dem Oszillator (5) und dem Eingangssignal gebildet wird in einer Mischeinrichtung (4); und daß eine Differenz zwischen dem Oszillator-Ausgangssignal und dem Meßsignal gebildet wird in einer zweiten Mischeinrichtung (12), wobei somit zwei Niederfrequenzsignale gebildet werden, diese Signale in einem Phasendetektor (9) verglichen werden im Hinblick auf die Phasenposition, so daß der Detektor (9) die erste Spannung abgibt, wenn es eine Phasendifferenz gibt, aber wenn es Phasengleichheit gibt, er eine Nullspannung abgibt.
  2. Anordnung nach Anspruch 1, dadurch gekennzeichnet, daß der Oszillator gesteuert ist durch die zweite Spannung, die durch das Signal erzeugt wird, dessen Frequenz die Differenz zwischen der Eingangssignalfrequenz und der Oszillatorsignalfrequenz ist, wobei dieses Signal eine Ausgangsspannung von einem Frequenzdetektor (16) verursacht, die die zweite Spannung ist, und es einen Integrator (17) gibt zum Vergleichen dieser zweiten Spannung mit einer Referenzspannung, so daß, wenn die Differenz konstant ist, der Oszillator bei der gegebenen Frequenz verbleibt.
  3. Anordnung nach Anspruch 1, dadurch gekennzeichnet, daß das Eingangssignal zu dem Resonanzmodul durch einen Isolator (1) läuft, der nur Signale in Richtung auf das Resonanzmodul durchläßt.
  4. Anordnung nach Anspruch 1, dadurch gekennzeichnet, daß ein Bandpaßfilter (6) nach der Mischeinrichtung 4 angeordnet ist und so eingerichtet ist, daß er den Durchgang des Signals erlaubt, das eine niedrige Frequenz in Relation zu der Frequenz des Referenzsignals hat.
  5. Anordnung nach Anspruch 1, dadurch gekennzeichnet, daß ein Bandpaßfilter (13) hinter dem Mischer (12) angeordnet ist, so daß es den Durchgang eines Signals erlaubt, das eine sehr niedrige Frequenz im Bezug zu der der Meßsignale (1', 2', 3' und 4') hat.
  6. Anordnung nach Anspruch 1, dadurch gekennzeichnet, daß der Oszillator gesteuert ist durch einen digitalen Code von dem Sender über eine Schaltung, die Frequenz künstlich erzeugt, die eine eingestellte Spannung zu dem Oszillator überträgt.
EP92903213A 1991-01-09 1992-01-08 Justierungsvorrichtung für resonanzmodul Expired - Lifetime EP0566640B1 (de)

Applications Claiming Priority (3)

Application Number Priority Date Filing Date Title
SE9100065A SE467901B (sv) 1991-01-09 1991-01-09 Anordning vid avstaemning av resonansmodul
SE9100065 1991-01-09
PCT/SE1992/000004 WO1992012577A1 (en) 1991-01-09 1992-01-08 Tuning means for resonance module

Publications (2)

Publication Number Publication Date
EP0566640A1 EP0566640A1 (de) 1993-10-27
EP0566640B1 true EP0566640B1 (de) 1996-11-13

Family

ID=20381570

Family Applications (1)

Application Number Title Priority Date Filing Date
EP92903213A Expired - Lifetime EP0566640B1 (de) 1991-01-09 1992-01-08 Justierungsvorrichtung für resonanzmodul

Country Status (5)

Country Link
US (1) US5374905A (de)
EP (1) EP0566640B1 (de)
DE (1) DE69215211T2 (de)
SE (1) SE467901B (de)
WO (1) WO1992012577A1 (de)

Families Citing this family (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US6246727B1 (en) 1996-07-10 2001-06-12 Allgon Ab Method and system for tuning resonance modules
SE507698C2 (sv) * 1996-07-10 1998-07-06 Allgon Ab Förfarande och system för avstämning resonansmoduler
SE514183C2 (sv) * 1999-01-27 2001-01-15 Ericsson Telefon Ab L M Inställningsarrangemang
KR100707221B1 (ko) * 2005-06-09 2007-04-13 광운대학교 산학협력단 광대역 주파수 합성기

Family Cites Families (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
GB955223A (en) * 1961-08-30 1964-04-15 Siemens Ag Automatic control device for a radio transmitter
JP2680005B2 (ja) * 1987-11-30 1997-11-19 株式会社日立製作所 シンクロトロン加速の加速方法
DE68926860T2 (de) * 1988-12-02 1997-02-20 Allgon Ab Verfahren und anordnung, die sich auf ein elektromechanisch gesteuertes resonanzmodul beziehen

Also Published As

Publication number Publication date
DE69215211T2 (de) 1997-03-20
EP0566640A1 (de) 1993-10-27
SE9100065L (sv) 1992-07-10
SE9100065D0 (sv) 1991-01-09
SE467901B (sv) 1992-09-28
WO1992012577A1 (en) 1992-07-23
US5374905A (en) 1994-12-20
DE69215211D1 (de) 1996-12-19

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